Research Memorandum

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Research Memorandum RM A50K07 NACA RESEARCH MEMORANDUM AERODYNAMIC STUDY OF A WING-FUSELAGE COMBINATION EMPLOYING A WING SWEPT BACK 63° - EFFECTIVENESS AT SUPERSONIC SPEEDS OF A 30-PERCENT CHORD, 50- PERCENT SEMISPAN ELEVON AS A LATERAL CONTROL DEVICE By Robert N. Olson and Merrill H. Mead Ames Aeronautical Laboratory Moffett Field, Calif. NATIONAL ADVISORY COMMITTEE FOR AERON AU TICS WASH INGTON January 18, 1951 Declassified April 8, 1957 1 NACA RM A50K07 NATIONAL ADVISORY COMMITTEE FOR AERONATITI CS RESEARCH MEMORANDUM AERODYNAMIC STUDY OF A WING-FUSELAGE COMBINATION EMPLOYING A WING 0 SWEP"r BACK 63 - EFFECTIVENESS AT SUPERSONIC SPEEDS OF A 30-PERCENT CHORD, 50-PERCENT SEMISPAN ElEVON AS A LATERAL CONTROL DEVICE By Robert N. Olson and Merrill H. Mead SUMMARY The effectiveness of a 5O-percent-semispan, constant-percent-chord elevon and of uppe~urface spoilers as lateral-control devices for a wing-fuselage combination employing a wing swept back 630 has been determined experimentally for the range of Mac.h numbers from 1.2 to 1.7 at a Reynolds number of 1.5 million. The results are compared with calculated values of the rolling-moment-effectiveness parameter CZ Q as obtained by the application of the linearized theory of supersonlc flow. For the elevon, results indicate that only about half of the rolling-moment effectiveness predicted by linear theory was realized. The variation of Mach number had little effect on the rolling-moment effectiveness of the elevon over the range investigated (Mach numbers of 1.2 to 1.7). Increasing angle of attack in the range of 00 to 100 had a moderate, adverse effect on the rolling-moment effectiveness of the elevon at a Mach number of 1.2; however, this effect diminished wi th increasing Mach number and became inappreciable in the range of 1.5 to 1.7 Mac.h number. The lateral-control characteristics of the elevon were little affected by variation of sideslip angle in the range from 50 to _5°. Elevon deflection produced small adverse yawing moments at positive angles of attack, w.hich were of suc.h small magnitude as to be of little concern. The upper-surface spOilers, having a maximum projection equal to the maximum wing-section thickness, were found to be inferior to the elevons for lateral control of this model because of a rapid loss in 0 effectiveness above an angle of attack of 4 • J 2 NACA RM A50K07 The present elevon was found to be more than adequate for rolling control of this wing-:fuselage combination if the wing were rigid; hovi­ ever, aeroelastic effects, computed from an approximate strip theory, were found to influence the rolling effectiveness of the elevon to the extent that structural considerations would be of prime importance in the final estimation of required elevon size. INTRODUCTION An investigation was made to determine means of attaining adequate lateral and longitudinal control for a wing-fuselage combination designed for efficient flight at supersonic speeds. This wing-fuselage combination, designed according to the theory advanced by J ones in ref­ erence 1, employed a wing of aspect ratio 3.5, taper ratio 0.25, and 630 sweepback of the leading edge. The results of wind-t unnel tests a t supersonic speeds to determine the effectiveness of a 3O-percent chord, 5O-percent-semispan elevon as a longitudinal control for this wing­ fuselage combination are presented (along with drag and hinge-moment data) in reference 2. The present report presents the results of a wind-tunnel investigation at supersonic speeds to determine the lateral­ control characteristics of this elevon. The lateral-control character­ istics of upper-surface, 5O-percent-semispan, outboard spoilers were also investigated. NOTATION All moment coefficients were referred to the stab ility axes wi th the origin located at the quarter-chord point of t he mean aerodynamic chord projected to the fuselage center line. rolling-moment coefficient (rolling moment) qSb damping-moment coefficient in roll; the rate of change of rolling­ moment coefficient C1 with wing-tip helix angle pb/2V, per radian C elevon rolling-moment-effectiveness parameter for constant angle of 1 o attack(dC 1 ) do a. Cn yawing-moment coefficient referred to quarter-chord point of mean aerodynamic chord (yaWing moment) qSb NACA RM A50K07 3 M Mach number (Via) R Reynolds number (pvc/~) S wing area~ square feet V airspeed, feet per second a speed of sound, feet per second b wing span~ feet b/2 (1 2 c dY), c wing mean aerodynamic chord 0 :feet b/2 f c dy o c local wing chord measured parallel to plane of symmetry, feet p angular velocity in roll, radians per second pb wing-tip helix angle, radians 2V q dynamic pressure (~V2), pounds per square :foot ~ angle of attack o:f :fuselage center line~ degrees ~ angle o:f sideslip, positive with right wing leading~ degrees 5 angle between wing chord and elevon chord, measured in a plane perpendicular to the elevon hinge line~ positive :for downward deflection with respect to the wing, degrees p mass density o:f air, slugs per cubic :foot ~ viscosity o:f air, slugs per foot-second Coefficients indicated with a prime (.) are uncorrected :for tunnel pressure gradient and flow inclination. APPARATUS AND TEST METHODS The investigation was conduct~d in the Ames 6- by 6-foot supersonic wind tunnel which is equipped with an asymmetric adjustable nozzle per­ mitting a variation in Mach number from 1.2 to 2.0 in the pressure range 4 NACA RM A50K07 of 2 to 20 pounds per s'luare inch absolute. However, due to certain vibration di:fficulties of the present model support system, the Mach number range is temporarily limited to a maximum of 1.7. The strain-gage balance and instrumentation are described in detail in reference 2. The model, pertinent dimensions of which are presented with a plan form sketch in figure 1, is shown mounted in the test section in the photograph of figure 2. The wing was untwisted, had 00 incidence, and was composed of NACA 0010 airfoil sections perpendicular to the leading edge. A ~ercent-chord elevon was mounted on the outboard 50 percent of the right wing panel. Spoilers, in heights up to the maximum wing­ section thickness, were constructed of aluminum alloy angles and were located successively at 40-, 50-, and 6o-percent-chord stations of the outboard half of the right wing panel. The wing and elevon were of solid-steel construction, while the fuselage was of hollo~teel con­ struction to permit the installation of the four-component strain-gage balance. A cutaway schematic drawing showing this installation is pre­ sented in reference 2. The fuselage was designed on the basis of mini­ mum wave drag for a given volume and length and had a fineness ratio of 12.5, including that portion of the body cut off to provide a method of attaching the model to the sting support. To shorte~ the testing time necessary for the lateral-control­ effectiveness investigation, the model was mounted in the test section with the plane of the wing placed vertically. With the model mounted in this manner, the present model support system permits continuous variation of the angle of sideslip during the test. Changing angle of attack, however, entailed changing the model support sting for each desired angle of attack. Side forces, rolling moments, and yawing moments were measured over a Mach number range from 1.2 to 1.7 at a Reynolds number of 1.5 million. The data were then transferred to stability axes and reduced to final coefficient form. Force measurements were made at nominal angles of sideslip of _50, -2.5°, 00 , 2.50 , and 50 for angles of attack of 00 , 0 0 5 1 and 10°. The elevon deflection was varied in 10 increments from 10° to -300 • The angle of sideslip of the model was determined optically by means of a cathetometer. The control-surface deflections, however, could not be determined during tests but were measured under stat ic conditions before each test and corrected for deflection under aero­ dynamic loading, using constants determined from static loading tests . The angle of attack was fixed for each test condition by us ing a sting bent to the desired angle. Since the angles of attack could not ------ ------------ NACA RM A50K07 5 be measured during the test, the angle of attack was measured initially under static conditions and corrected for deflection under aerodynamic load, using constants determined from static loading tests. REDUCTION OF DATA Since the force and moment strain gages were located inside the model, there were no direct foree tares due to aerodynamic forces on the sting. Effects of support interference, for the present investi­ gation, are confined to changes in base pressure and thus an effect on drag. (See reference 3.) Although the variations in stream curvature existing in the test section of the Ames 6- by 6-foot wind tunnel (discussed in reference 4) are such that lateral characteristics of a highly swept wing-body cam­ bination such as the present configuration, tested at Mach numbers other than 1.4, would be subject to some doubt, values of the incremental aerodynamic coefficients due to elevon deflection are reliable. Be cause of the axial variations in stream angle at Mach numbers above and below 1.4, however, it is difficult to determine the effective model angle of sideslip when testing with the plane of the wing vertical. Therefore, the angles of sideslip referred to in the report are nominal angles referenced to the borizontal plane and as such restrict the significance of the angle-of-sideslip eff ect s on the control-surface-effectiveness parameters to a qualitative indication as to t rends with Mach number.
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